Rotational Motion - Two spheres orbiting around a common barycenter

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Homework Help Overview

The discussion revolves around two spherical bodies of equal mass orbiting a common barycenter in a weightless environment, focusing on the relationship between orbital frequency and distance, as well as the dynamics of a weight attached to a spring in this system.

Discussion Character

  • Mixed

Approaches and Questions Raised

  • The original poster attempts to derive the frequency of rotation and the spring coefficient based on gravitational and centripetal forces.
  • Some participants question the assumptions regarding the resting length of the spring and the equilibrium position of the weight, suggesting that these factors could affect the spring coefficient.
  • Others express uncertainty about the interpretation of the problem and the implications of the weight's position relative to the barycenter.

Discussion Status

The discussion is ongoing, with participants exploring different interpretations and raising questions about the assumptions made in the problem. Some guidance has been offered regarding the potential indeterminacy of the spring coefficient based on the resting length of the spring.

Contextual Notes

There is mention of potential confusion due to language barriers, and participants are considering the implications of the weight's position affecting the center of mass of the system.

Rosengrip
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Homework Statement



Two spherical bodies with equal mass m1=m2=1000 kg are orbiting around a common barycenter in a weightless environment because of the gravitational attraction.

A: Show how the frequency of orbiting is related to the distance between two bodies.

B: We connect two bodies with a massless rod. There is a spring connected to the center of this rod (axis around which the bodies rotate) with a weight on one end. Mass of weight is 1 kg. What is the spring coefficient, if the weight doesn't move during rotation? Assume the frequency of rotation is one revolution per day.

C: Assume the weight attached to a spring is oscillating during rotations with small amplitudes. What is the spring coefficient, if the weight oscillates 12 times during 1 revolution?

Sketch for better understanding:
[URL]http://www.shrani.si/f/26/TO/4cz4TVm7/skica1.png[/URL]




Homework Equations


F = (Gm1m2)/r2
F = ks
Equations for oscillating motion

The Attempt at a Solution



A: Force of gravity is a centripetal force.

for body1: m1w2r = (Gm1m2)/R2 (r = distance for body1 to barycenter, R = distance between to bodies, w = angular velocity of body1)

Out of this equation I get the frequency of rotation for body1:

f = SQRT[ (Gm2) / (4R2rPi2) ]
It's the same for the other body.

B: Force of spring is a centripetal force

mw2s = ks (s = distance of weight from barycenter and the length of spring, m = mass of weight)

k = mw2

Here I didn't include both attractive forces from two bodies, which complicate things a bit. What I got here is way too simple so I'm pretty sure I'm missing something.

C: don't really have an idea how to do this, any tips would be cool :)

I'm pretty sure my soulution of A is right, not sure about B though. So I need someone to review this. Thanks.
 
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Rosengrip said:
B: We connect two bodies with a massless rod. There is a spring connected to the center of this rod (axis around which the bodies rotate) with a weight on one end. Mass of weight is 1 kg. What is the spring coefficient, if the weight doesn't move during rotation? Assume the frequency of rotation is one revolution per day.

Interesting. There's no mention of the resting length of the spring, nor of the equilibrium position of the weight from the center of rotation. I suppose one could come up with a formula for the spring coefficient which depends upon the distance of the equilibrium point from the barycenter and the resting length of the spring.

If the resting length of the spring is taken to be zero, then there will be no centrifugal force acting on the weight if it starts from there. So the spring coefficient could be any value! It's indeterminate.

If the spring constant is infinite (the spring is a rigid rod), then the weight is guaranteed not to move no matter what!

If the resting length of the spring is zero but the weight is nudged away from the center, then presumably it could settle down at a distance r from the barycenter that would depend upon the value of k. Your choice of either r or k will determine things.

I'm not sure how one is "expected" to interpret this. Is there an obvious choice?

Oh, by the way, I don't think it's valid to ignore the gravitational forces acting on the weight if its equilibrium position not a small fraction of distance between the spheres; The magnitudes of the acceleration terms become similar when r is more than about 15% of R.
 
The question is confusing in my native language too, I've sent an email to my mentor about this and I'll update it as soon as I get the answer.

Thanks for the reply though.
 
Rosengrip said:
The question is confusing in my native language too, I've sent an email to my mentor about this and I'll update it as soon as I get the answer.

Thanks for the reply though.

Thinking about it some more, I think that any position for the weight other than the center of mass of the two spheres is going to cause the assembly to have a new center of mass, and it won't be halfway between the spheres! This will make things a tad more complicated.

If one interprets the weight having zero motion as meaning not even orbiting about the center of mass, then the only possible choice would be for it to remain at the current center of mass.
 

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